Carrier wave signal system



April 4, 1950 A. 1.. MATTE CARRIER WAVE SIGNAL SYSTEM 2 Sheets-Sheet 1 Original Filed Oct. 20, 1942 lNVENTOR A. L. MATTE BY flaw ATTORNEY April 4, 1950 A. MATTE 2,502,971

CARRIER WAVE SIGNAL SYSTEM Original Filed 00. 20, 1942 2 Sheets-Sheet 2 [VET F IG. 2

A T TORN; V

UNITED STATES PATENT OFFICE CARRIER WAVE SIGNAL SYSTEM Andrew L. Matte, Summit, N. J assignor to Bell Telephone Laboratories, Incorporated, New York, N. Y., a corporation of New York Original application October 20, 1942, Serial No.

462,756. Divided and this application September 18, 1946, Serial No. 697,763

5 Claims.

This invention relates to a signaling system, and particularly to a receiver for a system in which mark-to-space and space-to-mark transitions are individually transmitted as discrete In multichannel signal systems where a plurality of discrete signal currents are amplified by the same line repeaters, the total amount of current on the line tends to approach the sum l rn in rr n i p l Whose durations 5 of the short time averages of the discrete signal are constant and independent of the length of currents when the number of channels is large. h r sp v marking and sp intervals As this determines the power capacity of the This application is a division of my copending line repeaters the economy of h System as 3 application, Serial No. 462,756, filed October 20, Whom is fi ted In systems of the types known now Patent patented On October previously the average amount of current i 1946- relatively high for the reasons that regulation ig i ggg i gg 3523 5 2 3 3: fi 5 333 31; and other purposes necessitate the transmission 0 rn the line r'n idle r markin order as to distinguish individual characters. i fg i g i i ig may oexist g g g sutch as submarme 17918 tively long time intervals where the majority of 2. 00 t F g con the telegraph circuits in such carrier systems g i, i' m a I k e pmzclp e will simultaneously transmit substantially the1r 333 gg i 53 i gi g i gig gi mifggifi tion may be particularly objectionable where both terval, and to suppress the current or reverse its iif g and i ip g i trapsg zi g f: $225 i i izg fi igg 55 reason that although the telegraph system may vals between transitions from space-to-mark and be transniuttmg no mtelhgence during the mark to space fic peak intervals of the telephone system, the

Impulse telegraph systems may be broadly ditelegraph System would tend to l Its K vided into two types; firstly, those in which mum demand P carrymg capamty of Space to mark and mark to space transitions the common carrier c1rcu1t. In other words the are generated at the sending and of the telegraph system would be imposing substantially transmission circuit; and secondly, those in which maxlmum fiemand on n' cntcult from such transitions are produced at the receivapower carrymg stand'pomt e s per10d Whe n mg end f the transmission circuit In the the telegraph system 1s transmitting no intelliusual type of alternating current systems in 35 gencewhich the carrier current generated at the send- The Present Invention contemplates a teleing end is sustained on the line for the entire graph System sufih that lmplllses of a e duration of marking or spacing transitions and rent are transmltted on a 11118 for tlmlng P suppressed during the converse operation, the poses o the duration of Such impulses P 86 average power obtaining on the line is relatively 40 from a time standpoint being y suifieient to substantial. Similarly, in a system in which the enable receiving apparatus to r spond to and inmarking or spacin transitions ar produced t clicate the occurrence of transitions, and such that the receiving end, the amount of current us no carrier current is transmitted on the line at tained on the line constitutes a relatively large Other times average. The present invention concerns a tele- The main Objec of t e n ention is to transgraph system arranged t t t t markmit telegraph code signals in one channel of a ing and spacing transitions only for the time inmultichannel carrier circuit such that substantervals required for the system to distinguish tially identical impulses of carrier current inditransitions, thereby utilizing substantially a cate only space-to-mark and marl -to-space minimum average amount of power to transmit transitions.

a given amount of intelligence.

Another object is to employ substantially a minimum amount of electrical power in order to transmit a given amount of intel.igence.

A further object is to eliminate all line current during intervals in which no intelligence is being transmitted.

Still another object is to obviate the necessity of maintaining current on the line during idle periods for level compensation purposes.

A still further object is to translate direct current signals of conventional type into transitional alternating current pulses.

Another object is to translate alternating current transitional pulses into conventional direct current signals.

In a specific embodiment, the present invention comprises sending and receiving loops operated by direct current and connected together by a line arranged to transmit alternating current. At the sending end, signals originate in the sending loop as periods of direct current flow corresponding to marks, and as periods of no current flow corresponding to spaces. The successive periods of current and no current in the sending loop are translated into pairs of direct current pulses of opposite polarity. The individual pulses are distinguished from each other on the basis of their polar characteristics by a pair of gaseous discharge devices and thereafter impressed successively on a modulator for translation into successively identical pulses of alternating current of certain frequency. At the receiving loop the successive alternating current pulses are rectified and then translated into suceessively identical steep wave front voltage pulses. These pulses are successively impressed on a pair of similarly poled gaseous discharge devices so arranged as to effect alternately in the receiving loop a period of direct current flow corresponding to a marking signal and a period of no current flow corresponding to a spacing signal. The corresponding marking and spacing signals occurring in both the sending and receiving loops are substantially identical in character.

A modification contemplates imparting distinctive magnitude characteristics to successive marking and spacing impulses of carrier current to avoid persistent inversion of the received signals which inversion might tend to result from the reception of an odd number of spurious carrier current pulses. In this modification, a pilot channel regulator located at the receiving terminal compensates for variations of line attenuation.

The invention will be readily understood from the following description taken together with the accompanying drawing in which:

Fig. l is a schematic circuit illustrating a specific embodiment of the invention, and

Fig. 2 shows the action at certain points of Fi 1.

Fig. 1 shows a combined sending and receiving terminal of an alternating current telegraph system arranged for full-duplex operation such that discrete impulses of alternating current are formed at the sending terminal of a transmission line and detected at a receiving terminal thereof. This system may be modified for half-duplex operation in a manner that will be hereinafter pointed out. It is to be understood that the arrangement of Fig. 1 is duplicated at the opposite end of the transmission line to provide a two-way carrier wave telegraph system.

Referring to Fig. 1, a sending loop is applied through a pulse-forming transformer l I and leads l2, I3 and M to the control grids of gaseous discharge tubes l5 and I5 arranged in push-pull relation. Included in the leads I2 and i4 are respective single pole switches I! and I8 whose function will appear subsequently and which normally rest on a pair of outer contacts l9, IS. The sending loop I9 embodies in series a key 20, a grounded source 2! of direct current potential and the primary winding of the pulse-forming transformer II.

The negative terminal of a source 26 of direct current potential, Whose positive terminal is connected to a point 21 common to the cathodes of both tubes 5 and I6, is applied to the control grids of both thereof, through lead [3, secondary windings of the pulse-forming transformer ll, leads l2 and i4, terminals I9, l9 and switches ll and H3. The anode circuit of tube 15 extends through anode resistance 28, primary winding 29 of transformer 34, source 3| of anode potential, lead 32, to the common point '21. The anode circuit of tube It is connected through anode resistance 28a, the positive terminal of the source 3 I, and lead 32 to common point 21.

The secondary windings 35 and 36 of the transformer 34 are respectively connected, via source 23 of direct potential, between the signal grids and cathodes of an electron discharge modulator 3? comprising pentagrid converter tubes 31a and 37b connected in push-pull relation. A source 42 of carrier current of certain frequency is connected between the common point 23a of the cathodes and the oscillator grids of both tubes 31a and 37b whose accelerating grids are connected together, and to a potentiometer arrangement consisting of serially connected resistances 42a and 420 bridged around direct current source 42b which supplies anode potential to both tubes 31a and 31b. The primary winding of input transformer 38 is serially connected in both anode circuits of the tubes 31a and 31b, while its secondary winding is applied to the input side of sending filter '39.

The tubes 31a and 31b and the carrier current source 42 serve to apply impulses of alternating current to the transmission line 4| under control of voltages present successively in the transformer 34 in a manner that will be hereinafter described. At all other times the source 23 serves to effectively bias the signal grids of the tubes 31a and 31b to suppress carrier current from the source 42.

Incoming transmission line 46 is applied to a channel receiving filter 4'1 through an input transformer 45 and a terminal regulating amplifier 48 whose function will be subsequently explained. The receiving filter 4'! is applied to an input winding of a transformer 49 whose split output winding is connected to the diode portion of a diode rectifier-triode amplifier tube 59 of which the triode portion is impressed across the input Winding of a transformer 5|. A source 52 ofdirect potential is applied through the primary winding of the transformer 5! to the anode of the triode. An R-C network 53 serves to supply biasing potential to the control grid of the triode in the usual manner. The diode portion of the tube 50 is arranged for full Wave rectification.

The output winding of the transformer 5! extends over leads 54 and 55 to the control grid- -cathode circuits of gaseous discharge tubes 56 and 51 embodied in receiving loop 44 as will pres- 'ently be explained, and whose control grids have connected in series therewith respective current limiting resistors 58 and 59. The anode circuit of the'tube 51 embodies common cathode .terminal 60, lead 6|, source 62 of direct potential, .point 10, lead 61, and resistance 68. The anode circuit of the tube E-is completed through either of the following two paths: (1) common cathode terminal 60, lead 6|, source 62 of direct potential, point I0, winding of sounder 63, key 64, winding 66 of transformer I4, the anode-cathode of the tube 56, and back to the common point 60; and (2) common cathode terminal 60, lead 6 I, source 52 of direct potential, point I0, lead 61, artificial line 14a, lead I 2, winding I3 of transformer I4, the anode-cathode of the tube 56, and back to the common point 60. The function of the path (2), called the artificial line path, will be hereinafter pointed out. The windings 65 and I3 constitute the primary winding of a pulseforming transformer 14 utilized for half-duplex operation in a manner that will be subsequently explained. A common source 80 of direct potential serves to bias the control grids of the tubes 56 and 57 through respective adjustable contacts 8| and 82. A capacitor I9 is applied across the anodes of both tubes 56 and 51.

Pilot Wave regulation embodies at the sending terminal of the line 4| a source 83 of alternating current of suitable frequency and fixed voltage applied through a series tuned circuit 84 across the input winding of the line transformer 49. A single pole single throw switch 84a is connected 'in series with the tuned circuit 84 and the pilot source 83. At the receiving terminal of the line 46, the received pilot wave is applied through transformer 85, series tuned circuit 86 and transformer 81 to a diode rectifier 88 arranged for full .direct potential is applied through the input Wind- .ing of the transformer 92 to the anode of the amplifier 9I. The operation of Fig. 1 will now be explainedin the following order: firstly, full-duplex with successive carrier current impulses having substantially identical magnitudes of envelopes; secondly, half-duplex with successive carrier current impulses having substantially identical magnitudes of envelopes; thirdly, full-duplex with successive carrier current impulses having different magnitudes of envelopes; and fourthly, halfduplex with successive carrier current impulses having difierent magnitudes of envelopes.

. In the operation of Fig. 1 arranged to produce and utilize a series of discrete carrier current im- Ipulses such that successive carrier current impulseshave substantially uniform or identical vmagnitudes of envelopes, it is to be understood that the two secondary windings 35 and 35 of the transformer 34 embody the same number of turns; that the contacts BI and 82 of the biasing source 80 at the receiving terminal are so adjusted that'the same magnitude of biasing voltage is simultaneously impressed on the control grids of both tubes 55 and 51; and that the sending key 64 of the receiving loop 44 is in-a closed position.

: When the sending key 20 is in the closed position, direct current flows steadily in the sending loop I0, and therefore through the primary winding of the pulse-forming transformer II. This will be assumed to be a marking condition. When the sending key 20 is in the open position, such direct current decays to zero. This will be assumed to be a spacing condition.

For the purpose of this explanation, it is assumed that the sending key 20 has been open for a period sumciently long that a steady state prevails in the system. This means that, as a consequence of a previous operation, gaseous tubes 16 and 51 are ionized; gaseous tubes I5 and 56 are deionized; and the voltages across the secondary windings 35 and 35 of the transformer 34 are substantially zero. Further, this means that the modulator 31 does not apply impulses of carrier current to the line M, as the biasing source 23 nullifies the effect of the carrier source 42 on the tubes 31a. and 31b. The building up and decay of direct current from the source 2i in the sending loop II] through the primary winding of the transformer II for the respective marking and spacing signals is illustrated in Fig. 2A. As is well known, a rising primary current causes the induction of a voltage in the secondary winding of the transformer II in one direction such that as the primary current reaches its steady state value the voltage in the secondary winding will have attained its maximum and then fallen to zero; and a falling primary current causes the induction of a voltage in the secondary winding of the transformer II in the opposite direction such that as the primary current reaches its steady state value the voltage in the secondary winding will have attained its maximum value and then fallen to Zero. The voltage in the output winding of the transformer I I will then be a series of a sharp pulses of alternately opposite polarity, one pulse at the start of each of the marking and spacing signals. Thus,

.the positive and negative voltage pulses for the respective marking or spacing signals in the sending loop I0 are illustrated in Fig. 2B. Accordingly, the positive and negative voltage pulses applied to the respective control grids of the gaseous tubes I5 and I5 to control ionization therein in the well-known manner are represented as the steep front pulses in Fig. 2B.

As the gaseous tube I5 is assumed to be deionized, the application of the voltage pulse of posithe sending key 2!) will institute ionization therein in the well-known manner. As the anode circuits of gaseous tubes I5 and I6 include individual resistors 28 and 28a respectively, and as the anodes of both latter tubes are directly connected by the capacitor 33, the starting of ionization in the tube I 5 causes a drop momentarily in the effective anode voltage applied to the gaseous tube I6 below a value at which ionization can be maintained. Hence, ionization in the gaseous tube I 6 is quenched. The application of the voltage pulse of negative polarity, Fig. 2B, in the control grid circuit of the gaseous tube I6, in response to a spacing actuation of the sending key 28 will institute ionization in the latter tube in the well-known manner. Here again the capacitor 33 and resistors 28 and 28a serve to reduce momentarily the effective anode voltage applied to the tube I5 below a value at which ionization therein can be maintained. Hence, ionization in the tube I5 is quenched. Thus the marking and spacing voltage pulses of opposite polarities, Fig.

, 2B, are effectively separated and serve to institute alternate ionization in the tubes I5 and I6 to produce a flow of current alternately in the anode circuits of the tubes I5 and I6 such that each anode current possesses the wave configuration illustrated in Fig'Q2C. Consequently, these anode currents are substantially identical in wave pat ternin-their 'respective circuits 'for bothmarking and-spacing actuations of the sending key 2B,-but flow in opposite directions with respect to;junc- -tion point 31a of these latter circuits.

ignition and extinction of ionization in the tube cause a flow of the anode current, Fig. 20, in thewinding-ZQ of the transformer. Thisserves to induce voltages-ineach of the windings 35 and '36 coupled to the winding 29. This is achieved in the manner'pointed out above in connection with the corresponding actionin theloop transformer 4 l. Consequently, the effective voltages applied to the signal grid-cathode circuits of the modulator tubes 3'laand'3lb and due toeach of therespective marking and spacing actuations of the sending key will have the wave shapes shown in Fig. 2B. -As the windings and 36 embody thesame number of turns, the magnitude of-the successive individual voltage pulses, Fig-23, will be substantially equal.

Due to the push-pull connection of the modulator tubes 31a and 311), the positive impulse of the voltage cycle, Fig. 23, serves to render the signal grid of the modulator tube 31a momentarilypositive. This institutes a flow of space current in the output circuit of the latter tube whereby thecarrier source 42 is enabled to transmit to the primary winding of its output trans- :foriner '38 an impulse of carrier current having the envelope shown as impulse (a) in Fig. 2E. The positive impulse of the voltage cycle, Fig. 2B, also appliedat the same time to the signal grid of the modulator tube 31b and has no eilect on the operation thereof except to drive its signal grid more negative momentarily. Conversely, the negative impulse of the voltage cycle, Fig. 213, has noeffect on the operation of the modulator tube-31a, except to drive its signal grid more negative -momentarily, while at the same time this negative impulse renders the signal ,grid'oi the modulator tube 312) positive momentarily. This institutes a flow of space current in theoutput circuit'of the latter tube whereby the carrier source 42 is enabled to transmit to the primary "winding of the output transformer 38 an impulse of carrier current having theenvelope illustrated asim'pulse (b) in Fig. 2E. Thus, the modulator 31 serves to convert the two voltage impulses of opposite polarity, Fig. 2B, into the two carrier currentimpulses (a) and (b), Fig. 2E, which impulses are provided substantially withequal envelopesfor the reason that the effects of the positive and"negative impulses, Fig. 2B, .on'the modulator 31 are substantially the same. Thus, in'Fig. 2E, the'impulse (a) corresponds to the space-to-mark transition while the impulse (b) corresponds to the mark-to-space transition. "The sending channel filter 39 rounds off the impulses of carrier current, 2E, to form'the carrier current impulses 2F which are transmitted to the line transformer 40 such that the impulses (c) and (d) ,Fig. 2F, correspond to'theimpulses (a) and (b), Fig. 2E, respectively.

At the receiving terminal the received impulses (c) and (d), Fig. 2F, are applied directly to the receiving'transformer 45, thence successively to the channel filter 41, transformer 49, and the -rectifier-amplifier 50. The regulating amplifier l8 and associated'circuits are not involvedin the mode of operation discussed at this point. In the output of the amplifier-rectifier 50, the amplified rectified marking and spacing carrierim- (pulses-appear as substantially identical: space-torepeat the initial spacing condition previously established in the sending loop key'20.

mark :and .mark-to-space :i'ectified impulses (e) and (I) .respectively, Fig. 2G. The space4o+mark andmark-tospace rectified impulses (e) and (I), Fig. .2G, are impressed through the transformer .51 onto the :control grids of the gaseous tubes 561and 51. 'At this point theispace-tmmark'and the imark-to-space impulses appear as the respectivelyidentical impulses (g) and (h), Fig. 2H. Each-of the latter impulses is impressed in .turnaon the control grids of both .tubes'56 and 51 at thesametime. Whichever tube-has ionizationequenched, 'that'tube will then have ionization .institutedtherein as the threshold bias .provided .by the "source V8!) is counteracted by the impulse-'(g) or (h),,Fig. 2H, by at least a certain minimum amount. "Due to the combinedaction of condenser 19, resistance 68,'and the effective resistance of .the receivingxloop .44, the institution of ionization in one ofthe tubes56 and 5'l'ser-ves to quench forthwith ionizationin theother of these tubes. As the tubes 56 and 51 are not arrangedin the push-pullrelation, the negative loops-of both theimpulses (g) and (h), Fig. 2H, in nowise affect the'ionization or deionization of either of" these tubes,:such action being influenced exclusively by the steep fronts of the positive portions of impulses (g) and (h), Fig. 2H.

'Asthe tube56 is assumedto be deionized, and thetube-51 to'be ionized, the'space-to-mark impulse .(g), Fig. 2H, impressed on the control grid oi both tubes 56 and 51 at the same'time serves .to institute ionization in the tube 56 whereupon ionization is quenched in the tube 51 in the usual manner. One .portion of anode current or-the tube56, therefore, flows in a-circuit extending frompositiveterminal of. source 62, branch .point 10, winding-0f. receiving sounder 63, key. 64, winding-GG oi transformer I4, anode-cathode of tube -56, common terminal 60 and lead 6| to the. negative terminal of .the source 62. From the branch .point 10 another and equal portion of anode currentof the tube 56.fiows .in. a circuit including lead S'Lartificial line 14a, lead "l2, .winding .13 of the transformer, anode-cathode circuitof .thetube 56, commonpoint 60, lead. 6|, source 62 ari'd'ba'ck to the' branch point 10. 'This flow of current serves to actuate the receiving sounder 53 "to a markingposition torepeat the initial marking condition. previously established in the sendingiloop key 20.

'Themark-to-space impulse (h), Fig. 2H, next impressed 'on the control grids'of both tubes "56'and 51 atthe sametime serves to institute ionization in'the tube 51, whereupon ionization is quenchedin the tube 58, so that anode current flows in a circuit comprising positive terminal ofrsource 62, branch point H1, lead 61, resistor "68, anode-cathode circuit of tube 51, common terminal 60, lead 6| and negative terminal of the isource62. As the extinction of ionization in the tube 56" interrupts the flow of energizing current for the -receiving sounder 63 in the previously traced receiving loop 44, such current interruptionwill'cause thesounder 63 to be actuated" in the'well -kn'own manner to a spacing position to V Hence, the-building up and decay of energizing-current inthe receiving loop 44 is illustrated in Fig. 2A.

"Thus the marking and spacing signalseifected -by the sending key 20 in the sending loop lll 'and comprising sustained variable periods of 4 direct current vIiiow interspersed with equally variable :"periodsof nofiow of direct current are subseiquentlyzestablished as substantially identical direct current signals in the receiving loop 44. Accordingly, both the initial and final signals are illustrated in Fig. 2A. 7 I

While the foregoing is based on closed and open periods of the sending loop [9, it is evident that polar signals would accomplish substantially the identical sequence of action.

For the operation of Fig. 1 on half-duplex such that successive space-to-mark and mark-tospace impulses are provided with substantially uniform or identical magnitudes of envelopes, the switches I7 and I8 are initially actuated to both inner contacts 95, 95. It will be understood that at the opposite terminals of the lines 41 and 46, not shown, is located equipment identical with that shown in Fig. 1, and further .that corresponding switches I! and. I8 thereat are likewise operated to corresponding innercontacts 95, 95. This switching operation effectively disconnects the sending loop it from the line 4|, and simultaneously therewith effectively conditions the loop M for both the transmitting of signals to the line 4i and the receiving of signals from the line 45 such that the received signals are isolated from the line 4|.

Such isolation is occasioned by the fact, as previously pointed out, that when a mark-tospace impulse is received from the line 45, the ionization of tube 55 is quenched so that no space current flows in either winding 65 or 13; whereas, when a space-to-mark impulse isreceived from the line 46 ionization is instituted in the tube 56 and equal amounts of space current are caused to flow in opposite directions in the windings 6B and it as indicated by the arrows. Equalization of these space currents maybe attained by suit--v able adjustment of the resistive characteristic of the artificial line Ma. Therefore, it is clear that during both the conditions of deionization and ionization of the tube 59 no voltage is produced in either of the secondary windings 96 or 9? of the transformer 74.

Half-duplex sending is initiated by operating the key M, to the closed position to transmit to the line 49 a space-to-mark impulse. During such operation, however, it is to be understood that the corresponding key located at the receiving terminal of the line 4|, not shown, is in the closed condition so that the corresponding tubes 56- andt'l thereat are in the ionized and deionized conditions respectively. Next, the key 64 is operated to the open position to transmit to the line ll a mark-to-space impulse. Such operations of the key 94 achieve precisely the same sequence of operations as that hereinbefore explained in connection with the corresponding operations of the key 29 in the case of full-duplex operation, whereby impulses of carrier current, Figs. 2E and 2F, are caused to be transmitted to the line 4|.

Thus, primary winding 66 of transformer-14 corresponds to the primary winding of the transformer H, while secondary windings 96 and 91 are connected to the gaseous discharge tubes l5 and it in exactly the same electrical relation with respect to the primary winding 66 as the secondary winding of the transformer ll bore formerly to the primary winding of the latter transformer in the case of full-duplex operation. Tube 56 is. held in the ionized condition when the key 94 is in the open position by the fact that a voltage is applied to the anode of the tube 56 .over a path comprising positive terminal of source 52, branch point it, artificial line 14a,

lead 2. primary Wi in 3. ano -c t o e.

tube 55, common terminal 69 and lead 6| to the negative terminal 1 of the source 62. As the amount of space current flowing in the next previously traced circuit is substantially constant, as distinguished from the gradual build-up and decay of space current in the primary winding 66, no voltage is induced in the associated secondary windings 96 and 9?. As a consequence there is novoltage to effect the production of impulses of carrier current from the carrier source 42 in the rnanner explained above.

If the distant operator wishes to break, he actuates his key 64 to the open position. This efiectively transmits a mark-to-space impulse over the line 46 whereby, in Fig. 1, ionization is instituted in the tube- 51 and ionization in the tube 56 is quenched. This efiectively opens the loop 44 in 1. thereby rendering the operation of key 64 in Fig. 1 further ineffective to transmit signals. Such-condition of'the loop 44 in Fig. 1 is instantly recognized by the operator of the key M in Fig. 1 by reason of the non-responsiveness of his sounder 63 in Fig. 1.

In the operation of- Fig. 1 on the'basis of fullduplex with successive space-to-mark and markto-spaceimpulses having diiierent magnitudes of envelopes, it is to be understood that initially the number of turns of the secondary winding 36 of the transformer 34 is so adjusted as to effect a predetermined difference between the magnitude of the voltage produced by this winding with reference to the magnitude of the voltage produced by-thesecondary winding 35 of the transformer 34; and further that the movable terminals 8-! and 92 of the biasing source are sci-adjusted as to-apply predetermined difierent amounts of biasing voltage to the control grids of the receiving tubes 56'and 51 so as to be commensurate with the magnitudes of the voltages applied to the. signal grids of the tubes 31a and 31b embodied in the. impulse modulator 31 for reasons that will presently appear.

The performance of the-transmitting end of the system of Fig. 1 including the operations of the key 29 and the successive ionization of the gaseous discharge tubes i 5 and I5 due to the space-to-m'ark and mark-to-space transitions is identical with that previously explained for the full-duplex operation of Fig. 1 in the case where the successive carrier impulses possess substantially identical magnitudes of envelopes; and therefore the wave shape of the space current flowing in the primary winding 29 of the transformer 34 is illustrated in Fig. 2C. However, as the. number of turns of the secondary winding 35 is assumed tobe larger than the number of turns oflthe secondary winding 35, the space-to-mark transitions which initiate the ionization of tube I5. and the mark-te-spacetransitions, which cause the ionizationof the tube It, are converted into the diiierent relative magnitudes of voltage impulses illustrated in Fig. 2K. Hence, in Fig.

2K, the impulse (u) is effected by the secondary winding 35 while the impulse (v) is effected by the secondary winding 36.

As in the case of duplex operation described above, the voltage impulses (u) and (12), Fig. 2K, cause the modulator tubes 377a and 31b respectively, to draw space current alternately whereby the carrier source 42 is enabled to supply the respective carrier current impulses (k) and (i), Fig. 2L, to the output winding of the transformer 38.v In this connection .it will be noted that the larger positive-impulse, Fig. 2K, enables thetubearla to transmit the largercarrier current impulse (76'), Fig. 2L, while the smaller negative impulse, Fig. 2K, enables the tube 31b to transmit the smaller carrier current impulse (7'), Fig. 2L. The carriercurrentimpulses (k) and (7'), Fig. 2L,- appear as the impulses (m) and (n), Fig. 2M, respectively; on'- the line 4| which impulses possess diflerent relative magnitudes of envelopes.

The carrier current impulses (m') and (n) Fig. 2M, are received over the line 45- and successively applied to the rectifier-amplifier 50 which eilects in the input winding of the transformer 51 the corresponding unidirectional impulses and ('p)'-, Fig; 2N In the output winding'o'fthetransformer the two unidirectional impulses (0) and (p), Fig. 2N, assume the respective configurations (s) and (t), Fig; 2P, and are impressed alternately and successively on the control grids ofboth tubes 55" and 51 at the same time. As the biasingvol'tage' applied to the control grid of the tube 55 is larger than that impressed on the controlgrid of the tube 51 as previously pointed out, only the impulse (s), Fig. 2P, is capable of instituting ionization in the tube: 56, the impulse (t), Fig. 2P, being inadequate for this purpose: It is to be noted that the impulse Cs), Fig. 21?, is also suflicient to institute ionization at thesame time in the tube 51, but as the latter tubeis already ionized due to a previously received mark-t0- spaee transitional impulse ('assumed), the effect of the impulse ('s), Fig. 2P, on the tube 51 is nil. The receiving tubes 55 and 51 are, therefore, actuated to cause the sounder 63 embodied in the loop 44' to reproduce themarking and spacing signals of the sendin key 20 in the manner hereinbe'fore described in connection with the fulldunlex operation of Fig; 1.

In the operation of Fig. l on half-duplex with successive carrier current impulses provided with magnitude discrimination, the aforementioned adjustment of the relativenumber of turns of the secondary windings 35' and 35' of the transformer 34, and the different magnitudes of biasing voltage impressed on the control grids of the receiving tubes 56 and 51 are maintained identical with the above-mentioned operation of Fig. 1 on full-duplex with magnitude discrimination. The operation of Fig. 1 on half-duplex with magnitude discrimination is the same as the previously described operation of Fig. I on half-duplex, except in the former operation. the successive carrier current impulses are provided with different magnitudes of envelopes. For the purpose of this illustration, the space-t'o-ma'rk impulses are provided with the larger envelopes and the markto-space impulses with the smaller envelopes. Therefore, the receiving terminal in Fig. 1 is arranged to discriminate between the carrier current impulses of diflerent magnitudes of envelopes exactly in the manner set forth hereinbefore in connection with the full-duplex operation of Fig. 1 with magnitude discrimination as illustrated in Figs. 2K, 2L, 2M, 2N and 2P.

The carrier current impulses of diiferent magnitudes of envelopes, Fig. 2M, prevent permanent turnover between spacing and marking functions of Fig. 1 when the turnover is occasioned by receiving an odd number of false impulses due to interference in a manner that will be presently explained. According to the above explanation, the institution of ionization in the sending tube I5 results in the institution ot'ionization in the receiving tube 56 while institution of ionization in the sending tube l6 results in the institution of ionization in the receiving tube 51. If tube 57 is Tube=lonized Case Magnitude of Emu No False P Before In. After:lntcrterfercnce ierence 1 Lessthan'v'. Either No change" No cflcct; 2.. Greater. than? v, 57 D lessthanV. 3; do 41...- Greater-than V 51. 0

In the last three cases, the effect of the next legitimatepulse as follows:

Tube Ionized Magnitude Case After Pulse No. g z .Belorc Arrives Result Pulse: Al'l'lVBS' .Actual Desired 6 1Snmllcr 56. 57 57' Sequencerostomd; 7.... do' 57. 57 57 Do. 8' Largei: 56 57 56 Error. 9 do 5W 56' f 56 Sequence restored.

In case 8, the transition is incorrectly received; but since the next signal is perforce of the smaller magnitude, it finds tube 51, which it should ionize, already in that condition, and since its" magnitude is insufiicient to ionize 56 the normal sequence is restored forthwith.

In the operation of Fig. l with magnitude discrimination as above explained, pilot wave regulation provides the space-to-mark and mark-tospace impulses arriving at the primary winding of the receiving transformer with substantially the same relative magnitudes of envelopes that theseimpulses had when they were applied to the sending terminal of the line 4|. Such regulation prevents the mark-to-space impulse of the lesser magnitude of envelope, Fig. 2M, from instituting ionization in the tube when the attentuation of line 4| is relatively low; or the space-to-mark impulse of the greater envelope. Fig. 2M, from failing to institute ionization in the tube 56' when the attentuation of line 4| is relatively high; such regulation also has the further advantage of minimizing the efiects of interference on line 4| or 46.

In the operation of the specific pilot wave regulator illustrated herein, a pilot alternating current wave of suitable frequency provided by the source 83 is applied through the series tuned circuit 84 and line transformer 40 to the sending end of the line 4|. At the receiving end of the line 45, this pilot wave is rectified in the rectifier 88 and the rectified voltage across the resister 19 is utilized to control the gain of the variable mu amplifier 9|. As the pilot wave undergoes the same line attenuation as the transmitted space-to-mark and mark-to-space impulses, the receiving terminal amplifier 48 serves to maintain the envelopes of these impulses substantially at desired relative magnitudes as i1- lustrated in Fig. 2M. The switch 84a may be utilized to disconnect the pilot source 83 from the line 4| during intervals when no intelligence is being transmitted.

In the above-explained operations of Fig. 1 on the basis of both full-duplex and half-duplex, both with and without magnitude discrimination, the successive impulses of carrier current are transmitted on the line for timing purposes only, the durations of such impulses being, from a time standpoint, only sufiicient to allow the receiving apparatus to respond to and indicate the occurences of transitions. Hence, carrier current is utilized only for the purpose of transmitting intelligence, and is disconnected from the line during other periods. In the latter periods, it is obviously unnecessary to transmit pilot current for regulation purposes; and therefore pilot current may also be utilized only during intervals when carrier current is being utilized to transmit intelligence and may be disconnected from the line during other periods.

Although the invention has been illustrated in connection with the use of metallic lines and a manually operated sending key, it is obvious that the invention may be expeditiously utilized in radio signaling systems as well as telegraph printers to produce marking and spacing impulses in systems involving metallic lines or radio systems. Further, it is to be understood that individual carrier current impulses can be interchanged to represent either mark-to-space or space-to-mark transitions without aiiecting the performance of the system.

What is claimed is:

1. An alternating current receiving signal system comprising a line transmitting impulses of alternating current having predetermined relative magnitudes for representing space-to-mark and mark-to-space transitions, each impulse representing one transition, said line transmitting no impulses when said transitions are withheld therefrom, a telegraph instrument, and means for connecting said line and instrument in circuit whereby said instrument is operated to repeat the transitions represented by the carrier impulses on said circuit line, said circuit means comprising means for translating the impulses received from said line into sharply peaked pulses having at least a certain polarity and predetermined relative magnitudes, and two ionizable devices, said circuit means being adapted to ionize and deionize said devices alternately in response to sharply peaked pulses of said certain polarity for controlling the flow of current in said instrument, said circuit means being arranged to maintain one device in the deionized state and the second device in the ionized state when said transitions are withheld from said line whereby no current is caused to flow in said instrument, said circuit means being activated by a sharply peaked pulse of said certain polarity and predetermined magnitude to ionize said one device and to deionize said second device to institute a flow of direct current in said instrument whereby said instrument is operated to repeat the transition represented by the alternating current impulse translated into said last-mentioned pulse, and said circuit means be- 14 by said instrument is operated to repeat the transition represented by the alternating current impulse translated into said last-mentioned pulse.

2. A signal system according to claim 1 in which said line transmits alternating current impulses having substantially equal magnitudes, said translating means translates the impulses received from line into sharply peaked pulses having at least said certain polarity and substantialy equal magnitudes, said circuit means is arranged to bias both said devices to the same extent, and said circuit means is so activated by sharply peaked pulses having said certain polarity and substantially equal magnitudes as to overcome the biases on said one and second devices to institute and terminate the ionization therein.

3. A signal system according to claim 1 in which said line transmits alternating current impulses having successively difierent magnitudes, said translating means translates the impulses received from said line into sharply peaked pulses having at least said certain polarity and successively dif ferent magnitudes, each of said ionizable devices includes a control grid, said circuit means is further adapted to bias the control grids of said devices to different amounts in such manner that said one device has its control grid biased to the larger amount, and said circuit means is activated by sharply peaked pulses having said certain polarity and successively different magnitudes to overcome the biases on the control grids of said one and second devices and thereby to ionize and deionize said one and second devices in such manner that said one device is ionized and said second device is deionized by the sharply peaked pulses having said certain polarity and the larger magnitude and further in such manner that said second device is ionized and said one device is deionized by the sharply peaked pulses having said certain polarity and the smaller magnitude.

4. A receiver for a carrier current telegraph signaling system comprising a transmission line for transmitting impulses of carrier current to identify signal transitions from space-to-mark and mark-to-space, said line transmitting no carrier current impulses when intelligence is being withheld therefrom, means for translating the carrier current impulses received on said line into relatively sharply peaked impulses of at least positive polarity, a telegraph instrument having an operating winding, a pair of gaseous discharge devices each including a cathode, a control grid and an anode, and means for connecting the anode and cathode of one of said devices, when ionized, in a series circuit with said operating winding and for connecting the anode and cathode of the second of said devices, when ionized, in shortcircuit relation to said operating winding, said circuit means being adapted to bias the control grids of said devices to maintain said one device in the deionized state and said second device in the ionized state when intelligence is being Withheld from said line whereby no current is caused to flow in said operating winding, said circuit means being adapted to alternately ionize said devices in response to sharply peaked pulses of said positive polarity only, said circuit means being adapted to apply to the control grids of both said devices the sharply peaked pulse of positive polarity due to a carrier impulse received from said line to overcome the bias on the control grid of said one device to cause said one device to ionize and said second device to deionize, said one device in the ionized state and said second device in the deionized state connecting the anode and athc l f: sa d e dev ce nv ser es sc a ica be aid q e a i erw nd n r q in u e a 10 ,11 rent he in re y aid n i nti ac uat to v reproduce the transition representedby the last-mentioned carrier; impulse, said circuit means being adapted to-ap lyto the control grids of both said devices the sharply peaked pulse of positive polarity due to the next; succeeding carrier im-. pulse received from said line to overcome the bias onthe control grid Off saidsecond device to cause said second device to ionize and said one device to deionize, said second devicein the ionized state and: saidone device in the deionized state conmeeting the anode and cathode ofsaid second device in short-circuit relation to said operating winding to interrupt the flow of current therein whereby said instrument is actuated toreproduce thetransition represented: by said last-mentioned carrier impulse.

5, A receiver for a carrier current telegraph signaling; system comprising a line for transmit.- ting carrier current, impulses having successively different amplitudes torrepresent signaling transitions from space-.to-mark and mark-to-space, said=line transmitting no carrier current impulses duringidle periods, means for translating the carrier current impulses received on said line into sharply peaked pulses having at least positive polarity and successivelydifierent amplitudes, a pair-of gaseous discharge devices each including a control grid, a cathode and an anode, means forapplyingdifferent amounts of bias to said control grids in such manner that the control grid of said one device has the. larger bias applied thereto, a telegraph reproducer, and means forconnecting said line, translating means, devices and reproducer in circuit, said circuit. means being adapted to connect said cathode and anode of one device in series relation to. said reproducer when said one device is ionized to institute a flow of current in said reproducer, said circuit means being adapted to connect said cathode and anode of the second device in a short-circuit relation to said reproducerwhen said second device is ionized to interrupt the flow of current in said re- 4 producer, said circuit means being arranged with said biasing means to maintain said one device th pnized t te and; sa d we dev ce n the ionized state when intelligence, is beingwithheld from said line, said circuit means being adapted to ionize and deionize said devices alternately in response to sharply peaked pulses of positive polarity only, said circuit means applying the sharply peaked pulses of positive polarity to the control grids of said devices due to the carrier current impulses received on said line until the sharply peakedpositive pulse of, the larger amplitude overcomesthe larger bias on the control grid ofsaid one device whereby said one device is ionized and saidsecond device is deionized, said one device in the ionized. state connecting its anode and cathode in series relation to said reproducer to institute a flow'of current therein thereby causing said reproducer to repeatthe transition represented by the carrier current impulse translated into said last-mentioned sharply peaked positive pulse of the larger amplitude, said circuit means also applying the sharply peaked pulses to the control grids of said devices due to the carrier current impulses received on said line until the next succeeding sharplyrpeaked positive pulse overcomes the bias on the control grid of said second device whereby said second device is ionized and said one device is deionized, said second device in the ionized state connecting its anode and cathode in short-circuit relation to said reproducer to terminate the flow of current there.- in thereby causing said reproducer to repeat the transition represented by the carrier current impulse translated into said last-mentioned sharply peaked positive pulse.

ANDREW L.

REFERENCES GI TED The following references are of record in the file of this patent:

UNITED STATES PATENTS,

Number Name Date 1,936,947 Morganstern Nov. 28, 1933 2,012,837 Tear Aug. 27, 1935 2,266,401 Reeves Dec. 16, 1941 2,444,429 Cleeton July 6, 1948 

